Jump to
S1C2
Energy calculated at PBEPBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.415399 |
| Energy at 298.15K | -491.416149 |
| HF Energy | -491.415399 |
| Nuclear repulsion energy | 79.401692 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at PBEPBE/cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3588 |
3564 |
180.08 |
|
|
|
| 2 |
A' |
2004 |
1990 |
569.40 |
|
|
|
| 3 |
A' |
865 |
859 |
0.91 |
|
|
|
| 4 |
A' |
671 |
667 |
314.28 |
|
|
|
| 5 |
A' |
450 |
447 |
49.13 |
|
|
|
| 6 |
A" |
473 |
470 |
4.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4025.9 cm
-1
Scaled (by 0.9931) Zero Point Vibrational Energy (zpe) 3998.1 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBEPBE/cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.166 |
1.697 |
0.000 |
| C2 |
0.000 |
0.496 |
0.000 |
| S3 |
0.041 |
-1.082 |
0.000 |
| H4 |
0.510 |
2.450 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.2123 | 2.7862 | 1.0126 |
C2 | 1.2123 | | 1.5781 | 2.0197 | S3 | 2.7862 | 1.5781 | | 3.5629 | H4 | 1.0126 | 2.0197 | 3.5629 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
173.594 |
|
C2 |
N1 |
H4 |
130.184 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.133 |
|
|
|
| 2 |
C |
0.043 |
|
|
|
| 3 |
S |
-0.103 |
|
|
|
| 4 |
H |
0.193 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.082 |
1.585 |
0.000 |
1.919 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.323 |
2.906 |
0.000 |
| y |
2.906 |
-19.293 |
0.000 |
| z |
0.000 |
0.000 |
-25.135 |
|
| Traceless |
| | x | y | z |
| x |
-2.110 |
2.906 |
0.000 |
| y |
2.906 |
5.436 |
0.000 |
| z |
0.000 |
0.000 |
-3.326 |
|
| Polar |
| 3z2-r2 | -6.653 |
| x2-y2 | -5.031 |
| xy | 2.906 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.294 |
-0.208 |
0.000 |
| y |
-0.208 |
9.349 |
0.000 |
| z |
0.000 |
0.000 |
3.141 |
<r2> (average value of r
2) Å
2
| <r2> |
61.148 |
| (<r2>)1/2 |
7.820 |
Jump to
S1C1
Energy calculated at PBEPBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.410450 |
| Energy at 298.15K | |
| HF Energy | -491.410450 |
| Nuclear repulsion energy | 79.474333 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at PBEPBE/cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3828 |
3801 |
634.64 |
|
|
|
| 2 |
Σ |
2115 |
2100 |
615.71 |
|
|
|
| 3 |
Σ |
851 |
845 |
18.53 |
|
|
|
| 4 |
Π |
470 |
466 |
9.05 |
|
|
|
| 4 |
Π |
470 |
466 |
9.05 |
|
|
|
| 5 |
Π |
516i |
512i |
136.63 |
|
|
|
| 5 |
Π |
516i |
512i |
136.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3350.1 cm
-1
Scaled (by 0.9931) Zero Point Vibrational Energy (zpe) 3327.0 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBEPBE/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.685 |
| C2 |
0.000 |
0.000 |
-0.497 |
| S3 |
0.000 |
0.000 |
1.091 |
| H4 |
0.000 |
0.000 |
-2.681 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1878 | 2.7757 | 0.9963 |
C2 | 1.1878 | | 1.5878 | 2.1841 | S3 | 2.7757 | 1.5878 | | 3.7719 | H4 | 0.9963 | 2.1841 | 3.7719 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
180.000 |
|
C2 |
N1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.125 |
|
|
|
| 2 |
C |
0.063 |
|
|
|
| 3 |
S |
-0.156 |
|
|
|
| 4 |
H |
0.218 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.925 |
2.925 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.093 |
0.000 |
0.000 |
| y |
0.000 |
-25.093 |
0.000 |
| z |
0.000 |
0.000 |
-15.790 |
|
| Traceless |
| | x | y | z |
| x |
-4.652 |
0.000 |
0.000 |
| y |
0.000 |
-4.652 |
0.000 |
| z |
0.000 |
0.000 |
9.303 |
|
| Polar |
| 3z2-r2 | 18.606 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.119 |
0.000 |
0.000 |
| y |
0.000 |
3.119 |
0.000 |
| z |
0.000 |
0.000 |
9.162 |
<r2> (average value of r
2) Å
2
| <r2> |
61.315 |
| (<r2>)1/2 |
7.830 |